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81)]. This means that, when incompletely eliminated, the peaks of isolated carbons will be "axial" (dotted circles on the zero frequency line of domain ∆). We also note that MT(cpl) is phase modulated with respect to td and amplitude modulated with respect to ∆. Consequently, mirrorimage peaks will appear at frequencies − Ω14. This reduces the intensity of the displayed signals and imposes restrictions on the choice of the transmitter frequency, increasing the size of the data matrix. A modified sequence has been proposed to obtain phase modulation with respect to ∆, the analog of a quadrature detection in domain ∆.

The fast one has gained p /2 and the slow one has lost p /2. As a result, the two vectors (of unequal magnitude) are now coincident. 43) confirm that at time t(8) both matrix elements d*12 and d*34 have the same phase factor, exp(iWCD2). 59) represents the enhancement of the carbon magnetization by polarization transfer. This could not be even guessed from the vector representation. Nothing remarkable happens after the end of D2. The proton decoupler is turned on and the carbon magnetization is precessing as a whole during the detection time td (no spreadout of the fast and slow components).

5. 5. Fast and slow labeling. , they are fast. Those in states 2 and 4 are slow. Likewise, carbons in states 1 and 2 are fast, those in states 3 and 4 are slow. 54), at t(0) half of MzH is due to fast protons (d11 - d33) and the other half to slow protons. 6 with 13 and 24, respectively. For carbon, it is 12 and 34. Speaking of C-H pairs, a proton can add or subtract to the field "seen" by the carbon. Therefore the carbon will be fast if it pairs with a spin-up proton or slow if it pairs with a spin-down proton.